2010
DOI: 10.1063/1.3393777
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Phase diagram of a tetrahedral patchy particle model for different interaction ranges

Abstract: We evaluate the phase diagram of the Kern-Frenkel patchy model with four interaction sites for four different values of the radial interaction range ͑all in the single-bond-per-patch regime͒ keeping the area of the interaction patches fixed. Four stable crystal phases are investigated, namely diamond cubic ͑DC͒, bcc, fcc, and plastic fcc. The DC is favored at low temperatures and pressures, while the bcc is favored at low temperatures and intermediate to high pressures. At low temperatures and very high pressu… Show more

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Cited by 127 publications
(185 citation statements)
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“…For narrow patch width, the four-patch phase diagram closely resembles the standard phase diagrams with a triple point below which the liquid state ceases to exist 19 . Unexpectedly, for wider patches the diamond crystal disappears from the phase diagram and a region in which the liquid is stable down to vanishing T opens up at intermediate ρ, in agreement with a numerical study of DNA-functionalized colloids 12,20 .…”
mentioning
confidence: 79%
“…For narrow patch width, the four-patch phase diagram closely resembles the standard phase diagrams with a triple point below which the liquid state ceases to exist 19 . Unexpectedly, for wider patches the diamond crystal disappears from the phase diagram and a region in which the liquid is stable down to vanishing T opens up at intermediate ρ, in agreement with a numerical study of DNA-functionalized colloids 12,20 .…”
mentioning
confidence: 79%
“…The global enthalpy minimum for this pressure value corresponds to, as previously reported in [12,5,8], a bcc-like structure that consists of two interpenetrating, but virtually non-interacting diamond lattices. This structure emerges in two different, but closely related versions: the particles of one diamond sublattice can be located exactly in the centers of the voids of the six-particle rings making up the other diamond sublattice ("b" in Figure 1) or the positions of the particles in each sublattice can be slightly shifted against each other ("a" in Figure 1).…”
Section: Structural Variations Along Isobarsmentioning
confidence: 99%
“…Before we start the discussion of structural variations along two selected isobars, we mention two structures, that have raised quite some interest in the literature [12,7,5], namely diamond cubic and diamond hexagonal phases (especially the former, which has potential use in the fabrication of materials with photonic band gaps [22]). In our calculations, these structures appear as corresponding to low-lying minima on the enthalpy landscape for very low pressure values, but as discussed in [5], are never stable for the values of the potential parameters we are using in this contribution.…”
Section: Structural Variations Along Isobarsmentioning
confidence: 99%
“…A particle with tetrahedral arrangement of patches is thought to be a natural building block that would favor local tetrahedral arrangement, consistent with a diamond lattice. However, both Monte Carlo (MC) and Molecular Dynamics (MD) simulations of this system reveal serious fundamental limitations of such an approach [4,[14][15][16][17]. First, there are two forms of the diamond lattices: cubic diamond (CD) and hexagonal diamond (HD), both having local tetrahedral arrangement, as shown in Figure 1.…”
Section: Introductionmentioning
confidence: 99%